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Break-off diameter

The mechanism of bubble formation by nucleation requires supersaturation of the dissolved gas [11-13] and a nucleus radius greater than the critical [7], The main sources of heterogeneous nucleation are usually surface irregularities capable of containing entrapped gas, e.g. pits and scratches. The bubbles typically develop over the electrode surface, grow in size until they reach a break-off diameter and subsequently detach into the electrolyte. After detachment, some residual gas remains at the nucleation site and another bubble will form at the same place [2,13,14], In most two-phase flow simulations [15-19], it is assumed that bubbles detach with a constant diameter, although from experiments [20,21] it is know that electrochemically formed bubbles show a size distribution. [Pg.110]

This increase of the portion of channel structure to the overall structure of the deposit in relation to the portion of holes to the overall structure is probably due to changes of the properties of the electroplating solution, caused by the dependences of the viscosity and surface tension of solution on temperature. As a result of this, the formation of holes becomes less possible and hence large holes appear only due to the edge effect, as can be clearly seen from Fig. 40c. It is obvious that the probability of the formation of the nucleus of such a structure decreases with lowering of the break-off diameter of the bubbles. [Pg.55]

The bubble break-off diameter depends on a current density and as it was shown by numerous experiments,71,76 77 it decreases with increasing current density. The fact that break-off diameter decreases with increasing current density is the result of varying electrode potential which affect the wettability and, hence, the contact angle supports the conclusion that (13) is a basic relationship to explain the dependence of the break-off diameter on the current density. Then, the bubble break-off diameter, d can be presented by... [Pg.56]

Finally, the analysis of the break-off diameter (or the diameter of the detached hydrogen bubble) can give an explanation why the change of hydrodynamic conditions in the near-electrode layer is achieved from the copper solution with the lower quantity of evolved hydrogen (i.e. from 0.15 M Q1SO4 in 0.50M H2SO4 at 800 mV... [Pg.57]

Liquid ammonia is stored in a tank at 24°C and a pressure of 1.4 X 106 Pa. A pipe of diameter 0.0945 m breaks off a short distance from the vessel (the tank), allowing the flashing ammonia to escape. The saturation vapor pressure of liquid ammonia at this temperature is 0.968 X 106 Pa, and its density is 603 kg/m3. Determine the mass flow rate through the leak. Equilibrium flashing conditions can be assumed. [Pg.154]

Shape of the liquid drop (Pendant drop method) The liquid drop forms as it flows through a tubing (Figure 2.11). At a stage just before it breaks off, the shape of the pendant drop has been used to estimate y. The drop shape is photographed and, from the diameter of the shape, y can be accurately determined. [Pg.25]

This relationship was verified at small heat fluxes only. Also a correlation for the average diameter of a bubble at the instant of break-off is available (F8) from experimental evidence for bubbles of steam and of hydrogen. [Pg.14]

Polyakov and co-workers [5] made an especially detailed study of the influence of the initial pressure and diameter of the vessel on the formation of nitric oxide in an explosion. They came to the conclusion that combustion takes place according to a branching chain mechanism and that the breaking off of the chains in the volume, i.e., the reaction of the active centers with... [Pg.364]

FIG. 4.14. Bench-top accessories (a) and (b) are used to support long lengtlis of tubing (c), (d) and (e) are typical cooling racks made from wood (f) is a useful cutting aid. Small diameter tubes or capillary tubes, or rods are marked with the knife and placed in a notch so that the mark is directly above the edges a shaip blow with the back of the knife will cause tlie glass to break off cleanly at the mark. [Pg.23]

The effect of mass and heat transfer associated with the problem of the bubble evolution is also very interesting. In the case of mass transport, we can assume that at a given current density, or flux, N number of the adsorbed bubbles can be formed. At a given time tR, the diameter reaches a critical value rh after which it breaks off. We assume that the fresh electrolyte arrives at a similar concentration of that of the bulk, especially when the convective flux is large enough. We also consider that the mass transport is rate determining, so when the new electrolyte arrives it rapidly converts into the product. Under this consideration, it follows the second Fick s law ... [Pg.340]

Analytical models of pore collapse follow two approaches, termed hydrodynamic [162] or viscoplastic. In Mader s hydrodynamic model [162] (Fig. 17a), a steep planar shock front hits the upstream surface of an empty spherical pore of diameter d (for nanopores, gas inside the pore can be neglected [52,162]), it accelerating the free surface to velocity 2Up [5]. The pore s free surface undergoes hydrodynamic focusing [61,162]. A material spike strikes the downstream surface, causing impact heating. In molecular dynamics simulations, individual molecules from the upstream surface are observed to break off and strike the downstream surface [61,163]. The hydrodynamic time constant for pore collapse is approximately the material transit time across the pore. [Pg.169]

The phenomena of uniform drop formation from a stream of liquid issuing from on orifice were noted as early as 1833 by Savart [2] and described mathematically by Lord Raleigh [3,4] and Weber [5]. In this type of system that is based on their observations, fluid under pressure issues from an orifice, typically 40-80 pm in diameter, and breaks up into uniform drops by the amplification of capillary waves induced onto the jet, usually by an electromechanical device that causes the pressure oscillations to propagate through the fluid. The drops break off from the jet in the presence of an electrostatic field called the charging filed, and thus acquire an electrostatic charge. The charged drops are directed to their... [Pg.206]


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See also in sourсe #XX -- [ Pg.54 , Pg.55 , Pg.56 , Pg.57 ]




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